Pulsed laser diode driver

ABSTRACT

A pulsed laser diode driver includes an inductor having a first terminal configured to receive a source voltage. A source capacitor has a first terminal connected to the first terminal of the inductor to provide the source voltage. A bypass switch has a drain node connected to a second terminal of the inductor and to a first terminal of a bypass capacitor. A laser diode switch has a drain node connected to the second terminal of the inductor. A laser diode has an anode connected to a source node of the laser diode switch and a cathode connected to a bias voltage node. The laser diode switch and the bypass switch control a current flow through the inductor to produce a high-current pulse through the laser diode, the high-current pulse corresponding to a peak current of a resonant waveform developed at the anode of the laser diode.

RELATED APPLICATIONS

This application is a continuation of U.S. Pat. Application No. 17/648,907, filed Jan. 25, 2022, which is a continuation of U.S. Pat. Application No. 17/301,009, filed Mar. 22, 2021, which issued as U.S. Pat. No. 11,245,247 on Feb. 8, 2022, and which claims priority to U.S. Provisional Application No. 62/994,470, filed Mar. 25, 2020, and to U.S. Provisional Application No. 63/127,794, filed Dec. 18, 2020, all of which are incorporated by reference for all purposes.

BACKGROUND

Laser-based ranging systems, such as Lidar, often use a pulsed laser diode driver circuit to generate a short, high-current pulse, which is passed through a laser diode to emit a corresponding pulse of laser light. Reflected pulses of laser light are received by the Lidar system and used to determine a distance between the Lidar system and the point of reflection. Spatial resolution of Lidar systems is determined in part by the width of the pulse of laser light. Thus, it is usually desirable to generate a pulse of light having a width of about 5 ns or less. However, parasitic inductances of the pulsed laser diode driver circuit and the laser diode typically must be overcome to achieve the desired short pulse width. For example, many laser diodes have at least one bond wire which can contribute 1nH of inductance, thereby limiting a slew rate of the current pulse unless there is very high voltage. Thus, some conventional pulsed laser diode driver circuits use a high source voltage, often greater than 40 V- 100 V, to achieve the desired pulse width. Switching devices, such as GaN field-effect transistors (FET) are often used in conventional pulsed laser diode driver circuits as they can withstand such high voltages. However, pulsed laser diode driver circuits that use GaN technology may be more expensive, and/or may be more difficult to integrate with Silicon-based architectures.

SUMMARY

In some embodiments, a pulsed laser diode driver includes a first inductor having a first terminal and a second terminal. The first terminal of the first inductor is configured to receive a first source voltage, the first source voltage being based on a DC input voltage. A first source capacitor has a first terminal directly electrically connected to the first terminal of the first inductor to provide the first source voltage, and a second terminal electrically coupled to ground. A first bypass switch has a drain node that is directly electrically connected to the second terminal of the first inductor and a source node that is directly electrically connected to ground. A first bypass capacitor has a first terminal directly electrically connected to the drain node of the first bypass switch. A first laser diode has an anode and a cathode. The anode of the first laser diode is directly electrically connected to the second terminal of the first inductor and to the drain node of the first bypass switch. A first laser diode switch has a drain node that is directly electrically connected to the cathode of the first laser diode and a source node that is directly electrically connected to ground. The first laser diode switch and the first bypass switch are configured to control a current flow through the first inductor to produce a high-current pulse through the first laser diode, the high-current pulse corresponding to a peak current of a resonant waveform developed at the anode of the first laser diode.

In some embodiments, a pulsed laser diode driver includes an inductor having a first terminal and a second terminal. The first terminal of the inductor is configured to receive a source voltage. A source capacitor has a first capacitor terminal that is directly electrically connected to the first terminal of the inductor to provide the source voltage and a second capacitor terminal electrically coupled to a bias voltage node. A source switch has a first terminal that is directly electrically connected to a DC input voltage terminal and a second terminal that is directly electrically connected to the first capacitor terminal. The source switch is operable to charge the source capacitor when the source switch is enabled. A bypass switch has a drain node that is directly electrically connected to the second terminal of the inductor and a source node that is directly electrically connected to the bias voltage node. A laser diode switch has a drain node that is directly electrically connected to the second terminal of the inductor and to the drain node of the bypass switch. A laser diode has an anode that is directly electrically connected to a source node of the laser diode switch and a cathode that is directly electrically connected to the bias voltage node. A bypass capacitor has i) a first terminal directly electrically connected to the second terminal of the inductor and a second terminal directly electrically connected to the bias voltage node, ii) a first terminal directly electrically connected to the anode of the laser diode and a second terminal directly electrically connected to the bias voltage node, iii) a first terminal directly electrically connected to the second terminal of the inductor and a second terminal directly electrically connected to the second capacitor terminal of the source capacitor, or iv) a first terminal directly electrically connected to the anode of the laser diode and a second terminal directly electrically connected to the second capacitor terminal of the source capacitor. The laser diode switch and the bypass switch are configured to control a current flow through the inductor to produce a high-current pulse through the laser diode, the high-current pulse corresponding to a peak current of a resonant waveform developed at the anode of the laser diode.

In some embodiments, a pulsed laser driver includes an inductor having a first terminal and a second terminal, the first terminal being configured to receive a source voltage. A source capacitor has a first capacitor terminal directly electrically connected to the first terminal of the inductor to provide the source voltage and a second capacitor terminal electrically coupled to a bias voltage node. A source switch has a first terminal that is directly electrically connected to a DC input voltage terminal and a second terminal that is directly electrically connected to the first capacitor terminal. The source switch is operable to charge the source capacitor when the source switch is enabled. A bypass switch has a drain node that is directly electrically connected to the second terminal of the inductor and a source node that is directly electrically connected to the bias voltage node. A laser diode has an anode and a cathode, the anode being directly electrically connected to the second terminal of the inductor and to the drain node of the bypass switch. A laser diode switch has a drain node that is directly electrically connected to the cathode of the laser diode and a source node that is directly electrically connected to the bias voltage node. A bypass capacitor has i) a first terminal directly electrically connected to the second terminal of the inductor and a second terminal directly electrically connected to the bias voltage node, ii) a first terminal directly electrically connected to the second terminal of the inductor and a second terminal directly electrically connected to the second capacitor terminal of the source capacitor, or iii) a first terminal directly electrically connected to the anode of the laser diode and a second terminal directly electrically connected to the cathode of the laser diode. The laser diode switch and the bypass switch are configured to control a current flow through the inductor to produce a high-current pulse through the laser diode, the high-current pulse corresponding to a peak current of a resonant waveform developed at the anode of the laser diode.

In some embodiments, a pulsed laser diode driver includes multiple inductors, each inductor having a first terminal and a second terminal, the first terminal of each inductor being configured to receive a respective source voltage. The pulsed laser diode driver includes multiple source capacitors, each source capacitor corresponding to a respective inductor and having a first capacitor terminal directly electrically connected to the first terminal of that respective inductor to provide the source voltage and a second capacitor terminal electrically coupled to a bias voltage node. The pulsed laser diode driver includes multiple bypass switches, each bypass switch corresponding to a respective inductor and having a drain node that is directly electrically connected to the second terminal of that respective inductor and a source node that is directly electrically connected to the bias voltage node. The pulsed laser diode driver includes multiple laser diodes, each laser diode corresponding to a respective inductor and a respective bypass switch and having an anode and a cathode, the anode being directly electrically connected to the second terminal of that respective inductor and to the drain node of that respective bypass switch. A laser diode switch has a drain node that is directly electrically connected to the cathode of each of the laser diodes and a source node that is directly electrically connected to the bias voltage node. The pulsed laser diode driver includes multiple bypass capacitors, each bypass capacitor corresponding to a respective inductor and having a first terminal directly electrically connected to the second terminal of that respective inductor and a second terminal directly electrically connected to the bias voltage node. The laser diode switch and the multiple bypass switches are configured to control a respective current flow through each of the inductors to produce a respective high-current pulse through each of the laser diodes, each of the high-current pulses corresponding to a peak current of a resonant waveform developed at the anode of a respective laser diode.

BRIEF DESCRIPTION OF THE DRAWINGS

FIGS. 1A-1C are simplified circuit schematics of pulsed laser diode drivers of a first general topology, in accordance with some embodiments.

FIGS. 2A-2D show simplified plots of signals related to operation of the pulsed laser diode driver shown in FIG. 1A, in accordance with some embodiments.

FIG. 3 is a portion of an example switching sequence for operation of the pulsed laser diode drivers shown in FIGS. 1A-1C, in accordance with some embodiments.

FIGS. 4A-4D are simplified circuit schematics of pulsed laser diode drivers of a second general topology, in accordance with some embodiments.

FIGS. 5A-5D are simplified circuit schematics of pulsed laser diode drivers of a third general topology, in accordance with some embodiments.

FIGS. 6A-6D are simplified circuit schematics of pulsed laser diode drivers of a fourth general topology, in accordance with some embodiments.

FIGS. 7A-7E are simplified circuit schematics of pulsed laser diode drivers of a fifth general topology, in accordance with some embodiments.

FIGS. 8A-8B are simplified circuit schematics of pulsed laser diode drivers of a sixth general topology, in accordance with some embodiments.

FIGS. 9A-9B are simplified circuit schematics of pulsed laser diode drivers of a seventh general topology, in accordance with some embodiments.

FIGS. 10A-10B are simplified circuit schematics of pulsed laser diode drivers of an eighth general topology, in accordance with some embodiments.

FIGS. 11-12 show simplified plots of signals related to operation of the pulsed laser diode driver shown in FIG. 10B, in accordance with some embodiments.

FIGS. 13A-13I are simplified circuit schematics of high-repetition-rate pulsed laser diode drivers, in accordance with some embodiments.

FIG. 14 shows simplified plots of signals related to operation of the pulsed laser diode driver shown in FIG. 13I, in accordance with some embodiments.

FIG. 15 shows a simplified circuit schematic of a pulsed laser diode driver of a ninth general topology, in accordance with some embodiments.

FIGS. 16A-16B show simplified plots of signals related to operation of the pulsed laser diode driver shown in FIG. 15 , in accordance with some embodiments.

FIGS. 17, 18, 19, and 20 are simplified circuit schematics of pulsed laser diode drivers having an adjustable DC input voltage, in accordance with some embodiments.

FIGS. 21A-21B are simplified plots of signals related to operation of the pulsed laser diode drivers shown in FIGS. 17, 18, 19, and 20 .

DETAILED DESCRIPTION

In accordance with some embodiments, pulsed laser diode driver circuits disclosed herein (“pulsed laser diode drivers”), generate high-current (e.g., 40 Amp) ultra-short pulses (e.g., 1-5 ns) to emit a laser pulse from a laser diode using a tunable resonant circuit, as compared to conventional solutions that rely on fixed, and often unavoidable, parasitic capacitances and inductances of a circuit. The tunable resonant circuit provides easily tunable parameters which control a pulse width, a peak current, a charge time, a recovery time, a decay time, and other tunable parameters of the pulsed laser diode driver. Embodiments of a switching sequence to drive the pulsed laser diode drivers disclosed herein are operable to generate a resonant waveform at an anode of the laser diode to produce the high-current pulse through the laser diode, a voltage level of the resonant waveform being advantageously sufficient to support the high-current pulse and not of a voltage level that exceeds the voltage required to generate the high-current pulse.

Thus, embodiments of such pulsed laser diode drivers can advantageously generate the high-current pulses using a low input voltage (e.g., 6 V, 9 V, 15 V, etc.) and can thereby use Silicon-based switches, rather than GaN-based switches which are used by many conventional solutions. Any of the pulsed laser diode drivers disclosed herein can therefore be integrated into a single semiconductor die. Embodiments of pulsed laser diode drivers disclosed herein advantageously use a discrete inductor (e.g., a through-hole or surface-mounted component) intentionally added to the pulsed laser diode driver to generate a resonant waveform rather than relying on parasitic inductances (e.g., of the laser diode, of bond wires, or inter-circuit connections) of the pulsed laser diode driver. As a result, embodiments of the laser drivers disclosed herein are easily tunable and have a reproducible architecture. By contrast, conventional pulsed laser diode drivers often use a variety of techniques to overcome the effects of parasitic inductances of the pulsed laser diode driver and of the laser diode itself and therefore teach away from intentionally adding yet additional inductance to the pulsed laser diode driver. In addition to such intentionally added inductors, the pulsed laser diode drivers disclosed herein advantageously include a bypass capacitor that may be used by a designer to easily tune a desired pulse width emitted by the laser diode, as compared to conventional solutions which only have a source capacitor, or that only consider non-tunable parasitic capacitances of the pulsed laser diode driver. Once again, such conventional solutions teach away from adding yet additional capacitance to the pulsed laser diode driver. Because conventional solutions rely on parasitic capacitances and inductances of the conventional laser driver, modifying parameters such as a pulse width might require a redesign or re-layout of the conventional solution. By comparison, parameters, such as a pulse width, of the pulsed laser diode drivers disclosed herein can be tuned by simply changing a component value.

Multi-channel laser diodes are conventionally produced on a single monolithic substrate housed in a laser diode package. Conventionally, a single pin of the laser diode package is connected to all of the laser diode cathodes as a group (i.e., “common cathode”), whereas each laser diode anode is individually connected to a respective pin of the laser diode package. Pulsing each laser diode independently conventionally requires a switch in the laser diode anode current path to select which laser diode fires. However, an N-type switch conventionally requires a bootstrap circuit to level-shift a gate drive of that switch when the laser diode current path is enabled. Such bootstrap circuitry adds complexity and cost to a pulsed laser diode driver design. Thus, disclosed herein are embodiments of a multi-channel pulsed laser diode driver circuit for independently driving laser diodes of a common cathode multi-channel laser diode package advantageously using N-type switches without any bootstrap circuitry.

A repetition rate of a multi-channel laser diode driver, as well as of each of the pulsed laser diode drivers described herein, is limited by a charging time of each channel’s source capacitor which is described below. The pulsed laser diode drivers described herein create narrow (e.g., 1-5 nsec) high-current pulses (e.g., 40 amp) through a driven laser diode. The instantaneous power in the driven laser diode is therefore high (e.g., in the order of hundreds of watts). For many applications (e.g., Lidar), the duty cycle of the pulse is generally 0.01% or less to limit a total power dissipated in the laser diode, which results in an upper limit to a repetition rate. In conventional pulsed laser diode driver applications, a resistor is used to charge source capacitors during each cycle. In such conventional solutions, an RC time constant of charging circuits is typically not an issue because the duty cycle is so low. However, for applications that require a higher repetition rate for laser pulses, the RC time constant of conventional charging circuits creates an undesirable limitation. Thus, in any of the embodiments disclosed herein, each source resistor of a given laser diode driver may be advantageously replaced by an actively controlled source switch that quickly charges an associated source capacitor.

Typical resonant driver designs require a damping resistor to minimize ringing duration. However, the added damping resistor dissipates power which lowers the overall power efficiency of the design. Thus, in some embodiments, a pulsed laser diode driver is disclosed that advantageously switches a damping resistor into the resonant circuit during portions of a switching sequence during which the damping resistor critically damps ringing, and switches the damping resistor out of the resonant circuit during portions of the switching sequence when the damping resistor is not providing a positive benefit to the resonant circuit, thereby increasing an overall power efficiency of the pulsed laser diode driver as compared to one that includes a damping resistor for the entirety of a switching sequence.

For some applications, the amplitude of a high-current pulse delivered by a pulsed laser diode driver, such as any of those disclosed herein, may need to be adjusted in amplitude from pulse to pulse. Thus, in some embodiments, any of the pulsed laser diode drivers disclosed herein may be advantageously configured to adjust an amplitude of the high-current pulse delivered to one or more laser diodes on a pulse-to-pulse basis.

FIGS. 1A-C are simplified circuit schematics of pulsed laser diode drivers 101-103 of a first general topology to drive a laser diode using a low-side switch, in accordance with some embodiments. The pulsed laser diode drivers 101-103 each generally include a source resistor R_(S), a source capacitor C_(S) (i.e., a physical component that is not representative of a parasitic capacitance of another component), a damping resistor R_(Damp), an inductor L_(S) (i.e., a physical component that is not representative of a parasitic inductance of another component), a bypass capacitor C_(BP) (i.e., a physical component that is not representative of a parasitic capacitance of another component), a laser diode D_(L), a bypass switch M_(BP), and a laser diode switch M_(DL). The laser diode switch M_(DL) is configured as a low-side switch. Also shown is a controller 120, nodes 110, 112, a parasitic inductance L_(DL) of the laser diode D_(L), a DC input voltage V_(in), a source voltage V_(S) at the source capacitor C_(S), a current i_(LS) through the inductor L_(S), a current i_(DL) through the laser diode D_(L), a bypass switch gate driver signal GATE_(BP), and a laser diode switch gate driver signal GATE_(DL).

Topologies of the pulsed laser diode drivers 101-103 vary with respect to the placement of the bypass capacitor C_(BP). In each of the topologies of the pulsed laser diode drivers 101-103, a first terminal of the source resistor Rs is configured to be directly electrically connected to the DC input voltage V_(in). A first terminal of the source capacitor C_(S) is directly electrically connected to a second terminal of the source resistor R_(S), and a second terminal of the source capacitor C_(S) is directly electrically connected to a first terminal of the damping resistor R_(Damp). A second terminal of the damping resistor R_(Damp) is directly electrically connected to a bias voltage node such as ground. Thus, the second terminal of the source capacitor C_(S) is electrically coupled to the bias voltage node. A first terminal of the inductor L_(S) is directly electrically connected to the second terminal of the source resistor R_(S) and to the first terminal of the source capacitor C_(S). A drain node of the bypass switch MBP is directly electrically connected to a second terminal of the inductor L_(S), and a source node of the bypass switch MBP is directly electrically connected to the bias voltage node. An anode of the laser diode DL is directly electrically connected to the second terminal of the inductor L_(S), and a cathode of the laser diode D_(L) is directly electrically connected to a drain node of the laser diode switch M_(DL). A source node of the laser diode switch M_(DL) is directly electrically connected to the bias voltage node.

The bypass switch M_(BP) is configured to receive the bypass switch gate driver signal GATE_(BP) at a gate node, the bypass switch gate driver signal GATE_(BP) being operable to turn the bypass switch M_(BP) on or off based on a voltage level of the bypass switch gate driver signal GATE_(BP). Similarly, the laser diode switch M_(DL) is configured to receive the laser diode switch gate driver signal GATE_(DL) at a gate node, the laser diode switch gate driver signal GATE_(DL) being operable to turn the laser diode switch M_(DL) on or off based on a voltage level of the laser diode switch gate driver signal GATE_(DL). In some embodiments, the pulsed laser diode driver circuits disclosed herein include one or more bootstrap circuits or other level-shifting circuits to drive one or more high-side switches. Either or both of the bypass switch M_(BP) and the laser diode switch M_(DL) can be implemented as N-type switches or P-type switches. In some embodiments, the bypass switch M_(BP) and the laser diode switch M_(DL) are implemented as Silicon-based or Silicon-Carbide-based field-effect transistors (FETs). Two or more components described herein as having terminals that are directly electrically connected have a DC current path between the respective terminals of the two or more components. For example, a first and second component are not directly electrically connected via a capacitor or inductor connected in series between the first component and the second component.

As shown in the simplified circuit schematic of the pulsed laser diode driver 101 of FIG. 1A, in some embodiments a first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to the anode of the laser diode D_(L). In such embodiments, a second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in the simplified circuit schematic of the pulsed laser diode driver 102 of FIG. 1B, in some embodiments, the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to the anode of the laser diode D_(L). The second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp). As shown in the simplified circuit schematic of the pulsed laser diode driver 103 of FIG. 1C, in some embodiments, the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor Ls and to the anode of the laser diode D_(L). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the drain terminal of the laser diode switch M_(DL) and to the cathode of the laser diode D_(L).

In some embodiments, the pulsed laser diode drivers 101-103 are configured to receive the DC input voltage V_(in) having a voltage range from about 10 V to 20V, which is advantageously lower than an input voltage used by many conventional pulsed laser diode drivers. The inductor L_(S) is a physical component added to the pulsed laser diode drivers 101-103 (i.e., as opposed to a representation of a parasitic inductance caused by components or interconnections such as bond wires). Similarly, the bypass capacitor C_(BP) is a physical component added to the pulsed laser diode drivers 101-103 (i.e., as opposed to a representation of a parasitic capacitance). One advantage of using physical inductor and capacitor components rather than using parasitic inductances is that values of the inductor L_(s) and the bypass capacitor C_(BP) can be easily modified by a designer or even an end-user. By comparison, conventional designs that rely on parasitic reactances may require re-design and/or re-layout to change an operating parameter.

As disclosed herein, values of the DC input voltage V_(in), the inductance of the inductor L_(S), the capacitance of the source capacitor C_(S), the resistance of the damping resistor R_(Damp), and the capacitance of the bypass capacitor C_(BP) can advantageously be selected (“tuned”) to achieve a desired operation of the pulsed laser diode drivers 101-103 (e.g., a charge time, a pulse width, a pulse voltage, a pulse current). For example, a pulse width of the current i_(DL) flowing through the laser diode D_(L) can be tuned by adjusting the capacitance value of the bypass capacitor C_(BP). A peak current level of the pulse of current i_(DL) flowing through the laser diode D_(L) can be tuned by adjusting the source voltage V_(S) on the supply capacitor C_(S). A capacitance value of the source capacitor C_(S) can be tuned to adjust a timing delay of the current pulse and an upper range of the current i_(DL) through the laser diode D_(L). Resistance values of the damping resistor R_(Damp) are dependent on the capacitance value of the supply capacitor C_(S) and can be tuned within a range of values such that at a lower resistance, a lower frequency resonance of the pulsed laser diode drivers disclosed herein is underdamped (e.g., at about R_(Damp) = 0.1 Ohm), or is critically damped (e.g., at about R_(Damp) = 0.4 Ohm). The damping resistor R_(Damp) is operable to prevent current of the generated resonant waveform from becoming negative which could thereby enable a body diode of the bypass switch M_(BP) or the laser diode switch M_(DL). Although a resulting maximum current level of the current i_(DL) through the laser diode D_(L) is lower for the critically damped case, the current level can be easily adjusted by raising the voltage level of the DC input voltage V_(in). In other embodiments, the damping resistor R_(Damp) is removed entirely from the design (i.e., the second terminal of the source capacitor C_(S) is directly electrically connected to the bias voltage node). In yet other embodiments, the resistance value of the damping resistor R_(Damp) is set to zero Ohms.

In some embodiments, the DC input voltage V_(in) is about 15 V, the inductance of the inductor L_(S) is about 6 nH, the capacitance of the source capacitor C_(S) is about 100 nF, the resistance of the damping resistor R_(Damp) is about 0.1 Ohms, and the capacitance of the bypass capacitor C_(BP) is about 1 nF. In some embodiments, a voltage at the first terminal of the damping resistor R_(Damp) is received by the controller 120 to provide an indication of a current flow through the damping resistor R_(Damp).

In some or all of the embodiments disclosed herein, to produce around a 40 A high-current pulse through the laser diode (or laser diodes) D_(L), the DC input voltage V_(in) may range from 10-15 volts. In some such embodiments, the inductance of inductor L_(S) may range from 5-10 nH, the value of which determines the amount of flux delay to produce the required current. In some such embodiments, the inductance of the inductor L_(S) is selected to be an order of magnitude greater than a parasitic inductance of a printed circuit board (PCB) in which the pulsed laser diode driver is implemented. In some embodiments, the resistance of the damping resistor R_(S) ranges from 100-200 mOhm. A capacitance of the bypass capacitor C_(BP) determines the pulse width of the high-current pulse through the laser diode(s) D_(L), and in some embodiments ranges in capacitance from 1-5 nF. In some such embodiments, a capacitance of the supply capacitor C_(S) ranges from 25-100 nF depending on a peak current of the high-current pulse through the laser diode(s) D_(L) that is required or desired. The smaller the supply capacitor C_(S), the higher the DC input voltage V_(in) is needed to get the required or desired peak current of the high-current pulse through the laser diode(s) D_(L). In some such embodiments, a smallest capacitance value of the supply capacitor C_(S) that can still deliver the needed or desired peak current of the high-current pulse through the laser diode(s) D_(L) is selected because all the remaining energy after the high-current pulse is shunted to ground and is wasted, thereby lowering a power efficiency of the pulsed laser diode driver.

The controller 120 may be integrated with any embodiment of the pulsed laser diode drivers disclosed herein, or it may be a circuit or module that is external to any embodiment of the pulsed laser diode drivers disclosed herein. The controller 120 is operable to generate one or more gate drive signals having a voltage level that is sufficient to control one or more laser diode switches M_(DL) and one or more bypass switches M_(BP). Additionally, the controller 120 is operable to sense a voltage and/or current at any of the nodes 110 and 112 and at nodes that are similar to, or the same as, the nodes 110 and 112 as described herein, or at still other nodes of the pulsed laser diode drivers disclosed herein. The controller 120 may include one or more timing circuits, look-up tables, processors, memory, or other modules to control the pulsed laser diode drivers disclosed herein. Operation of the pulsed laser diode drivers 101-103 is explained in detail with respect to simplified plots 201-207 of FIGS. 2A-D and an example switching sequence 300 shown in FIG. 3 .

FIGS. 2A-2D show simplified plots 201-207 of signals related to operation of the pulsed laser diode driver 101 shown in FIG. 1A, in accordance with some embodiments. However, signals related to the operation of the pulsed laser diode drivers 101-103, 401-404, 501-504, 601-604, 701-705, 801-802, and 901-902 are similar to, or are the same as, those shown in the simplified plots 201-207.

The simplified plot 201 illustrates a voltage plot of the bypass switch gate driver signal GATE_(BP) 220, a voltage plot of the laser diode switch gate driver signal GATE_(DL) 221, a current plot of the current i_(LS) through the inductor L_(S) 222, a current plot of the current i_(DL) through the laser diode D_(L) 223, and a voltage plot of the source voltage V_(S) 224 at the source capacitor C_(S), all over the same duration of time. Details of these signals are described below. The voltage plots of the bypass switch gate driver signal GATE_(BP) 220 and the laser diode switch gate driver signal GATE_(DL) 221 have been level-shifted for readability, but are, in actuality, low voltage inputs. Additionally, the voltage plots of the bypass switch gate driver signal GATE_(BP) 220 and the laser diode switch gate driver signal GATE_(DL) 221 assume that the laser diode switch M_(DL) and the bypass switch M_(BP) are NFET devices. However, if PFET devices are used instead, the polarity of the bypass switch gate driver signal GATE_(BP) 220 and the laser diode switch gate driver signal GATE_(DL) 221 are inverted.

Upon receiving (e.g., from the controller 120) an asserted level of the bypass switch gate driver signal GATE_(BP) 220 at the gate node of the bypass switch M_(BP), the bypass switch M_(BP) is enabled (i.e., transitioned to an ON-state). Similarly, upon receiving (e.g., from the controller 120) an asserted level of the laser diode switch gate driver signal GATE_(DL) 221 at the gate node of the laser diode switch M_(DL), the laser diode switch M_(DL) is enabled. As highlighted in the plot 202, when the bypass switch M_(BP) is enabled, the rising current i_(LS) 222 begins to flow through the inductor L_(S), thereby building magnetic flux at the inductor L_(S). When the current i_(LS) 222 has reached a desired level (e.g., as determined by the controller 120 using sensed current, voltage, a timer circuit, or as determined by design constraints), a de-asserted level of the bypass switch gate driver signal GATE_(BP) 220 is received (e.g., from the controller 120) at the gate node of the bypass switch M_(BP), thereby disabling the bypass switch M_(BP) (i.e., transitioned to an OFF-state). As highlighted in the plot 203, when the bypass switch M_(BP) is disabled, the current i_(LS) 222 which has built up through the inductor L_(S), having no other current path, is redirected through the laser diode D_(L), causing a short (e.g., 1 ns - 5 ns), high-current (e.g., > 30 A) pulse to flow through the laser diode D_(L), thereby causing the laser diode D_(L) to emit a pulse of laser light. Because energy in the form of flux has been stored at the inductor L_(S), the high-current pulse i_(DL) that flows through the laser diode D_(L) can be significantly greater than the current i_(LS) that flows through the inductor L_(S). Values of the reactive components of the laser diode drivers disclosed herein can be advantageously selected to generate a desired current amplitude of the high-current pulse i_(DL).

After emission from the laser diode D_(L), the bypass switch M_(BP) is reenabled by an asserted level of the bypass switch gate driver signal GATE_(BP) 220, and the laser diode switch M_(DL) is maintained in an enabled state by an asserted level of the laser diode switch gate driver signal GATE_(DL) 221. As highlighted in the plot 204, the bypass switch M_(BP) and the laser diode switch M_(DL) are both advantageously maintained in the enabled state as the source voltage V_(S) 224 stored at the source capacitor C_(S) is discharged. As highlighted in the plot 205, while the bypass switch M_(BP) and the laser diode switch M_(DL) are maintained in the enabled state, the current i_(DL) 223 through the laser diode D_(L) (and importantly, through the parasitic inductance L_(DL) of the laser diode D_(L)) diminishes to zero. Thereafter, both the bypass switch M_(BP) and the laser diode switch M_(DL) are disabled by de-asserted levels (e.g., from the controller 120) of the bypass switch gate driver signal GATE_(BP) 220 and the laser diode switch gate driver signal GATE_(DL) 221. Because the laser diode switch M_(DL) is not disabled until a current through the parasitic inductance L_(DL) of the laser diode D_(L) has diminished to zero, a high voltage spike advantageously does not develop at the anode of the laser diode D_(L) as there is no rapid change in current through the parasitic inductance L_(DL). Because such high voltage spikes are advantageously mitigated, the laser diode switch M_(DL) does not need to be selected to withstand high voltages, thereby simplifying the design and reducing the cost of the pulsed laser diode drivers disclosed herein as compared to conventional solutions. Additionally, because such high voltage spikes are mitigated, the pulsed laser diode drivers disclosed herein do not require voltage snubbing circuits that are commonly used in conventional solutions, thereby further simplifying the design and reducing the cost of the pulsed laser diode drivers disclosed herein as compared to conventional solutions.

The high-current pulse 223 is a first and largest peak of the resonant waveform developed by reactive components of the pulsed laser diode driver circuit. These reactive components include the source capacitor C_(S), the inductor L_(S), the parasitic inductance L_(DL) of the laser diode D_(L), and the bypass capacitor C_(BP). In addition to the advantages described above, the bypass switch M_(BP) also reduces subsequent resonant waveform “ringing” of the resonant waveform after the high-current pulse 223 is generated. As shown in the plot 206, if a bypass switch gate driver signal GATE_(BP) 220′ is not asserted after a high-current pulse i_(DL) 223′ is generated, ringing occurs on the current i_(LS) 222′ through the inductor L_(S), on the current i_(DL) 223′ through the laser diode D_(L), and on the source voltage V_(S) 224′ at the source capacitor C_(S). As shown, the high-current pulse 223 through the laser diode D_(L) corresponds to a peak (e.g., maximum, or local maximum, amplitude) current of a resonant waveform of current i_(DL) 223′ developed at the anode of the laser diode D_(L).

As previously described, values of the source capacitor C_(S), the inductor L_(S) and the bypass capacitor C_(BP) may be advantageously selected or “tuned” by a designer to meet desired performance criteria of the pulsed laser diode driver disclosed herein. For example, a capacitance value of the bypass capacitor C_(BP) may be selected based on a desired pulse width of the current i_(DL) through the laser diode D_(L). The plot 207 shows the pulse 223 generated when the capacitance of the bypass capacitor C_(BP) is equal to 1nF, and a pulse 223″ generated when the capacitance of the bypass capacitor C_(BP) is equal to 4nF. In use cases where a wider pulse, such as the pulse 223″, is desired, the source voltage V_(S) may be raised accordingly. Additionally, in some embodiments, the width of the de-asserted portion of the bypass switch gate driver signal GATE_(BP) 220 is widened to accommodate a wider pulse.

FIG. 3 illustrates a portion of an example switching sequence 300 for operation of the pulsed laser diode drivers 101-103 shown in FIGS. 1A-B, in accordance with some embodiments, and as was described with reference to FIGS. 2A-C. However, the switching sequence 300 is similar to, or the same as, respective switching sequences related to the operation of other embodiments of the pulsed laser diode drivers disclosed herein, including but not limited to the pulsed laser diode drivers 401-404, 501-504, 601-604, 701-705, 801-802, and 901-902.

At a precharge step 301, the bypass switch M_(BP) and the laser diode switch M_(DL) are off (i.e., not conducting). During the precharge step 301, the source capacitor C_(S) is charged through the source resistor R_(S). At a preflux step 302, the bypass switch M_(BP) and the laser diode switch M_(DL) are transitioned to an ON-state, thereby allowing the current i_(LS) to flow through the inductor L_(S) to store energy in the form of magnetic flux at the inductor L_(S). Even though both of the switches (M_(DL), M_(BP)) are in an ON-state at the preflux step 302, the bypass path through the bypass switch M_(BP) will carry all of the current i_(LS) because a bandgap voltage of the laser diode D_(L) needs to be overcome to allow current to flow through the laser diode D_(L).

In some embodiments, the laser diode switch M_(DL) is transitioned to an ON-state after the bypass switch M_(BP) is transitioned to an ON-state. At a pulse generation step 303, the bypass switch M_(BP) is transitioned to an OFF-state while the laser diode switch M_(DL) is maintained in an ON-state, thereby generating the high-current pulse through the laser diode D_(L). When the bypass switch M_(BP) is transitioned to the OFF-state, voltage at the anode of the laser diode D_(L) rises quickly, until the bandgap voltage of the laser diode D_(L) is overcome and the laser diode D_(L) begins to conduct current. Because of a resonant circuit formed by the bypass capacitor C_(BP) and the parasitic inductance L_(DL) of the laser diode D_(L), the voltage formed at the anode of the laser diode D_(L) will advantageously rise as high as necessary to overcome the bandgap voltage of the laser diode D_(L) and will generally be higher than the source voltage V_(S).

At a discharge step 304, the bypass switch M_(BP) and the laser diode switch M_(DL) are maintained in an ON-state to drain charge stored at the source capacitor C_(S), thereby reducing the current i_(DL) through the parasitic inductance L_(DL) to advantageously eliminate a high voltage spike at the anode of the laser diode D_(L) when the laser diode switch M_(DL) is transitioned to an OFF-state. At step 305, the bypass switch M_(BP) and the laser diode switch M_(DL) are transitioned to an OFF-state, thereby returning to the precharge state at step 301. Because the source voltage V_(s) at the source capacitor C_(S) is completely discharged at the end of the discharge step 304, there is very little current through the laser diode D_(L). Thus, there is advantageously very little overshoot when the switches M_(DL), M_(BP) are transitioned to the OFF-state at step 305, thereby preventing damage to the laser diode D_(L) and the switches M_(DL), M_(BP). The time interval of the overall pulse and bypass signals is selected, in some embodiments, such that the source capacitor C_(S) is fully discharged before the switches M_(DL), M_(BP) are transitioned to the OFF-state at step 305.

Other topologies of pulsed laser drivers, having the same or similar advantages and having similar operation as that of the pulsed laser diode drivers 101-103, are disclosed below. The example topologies disclosed herein are not an exhaustive list of possible topologies that have the same or similar advantages and similar operation as that of the pulsed laser diode drivers 101-103. For example, one of skill in the art will appreciate that some modifications can be made while still adhering to the general principle of operation disclosed herein. Such modifications include placement of the bypass capacitor C_(BP), component values, and the addition of serially connected components that provide a DC current path.

FIGS. 4A-D are simplified circuit schematics of pulsed laser diode drivers 401-404 of a second general topology that is configured to drive two or more laser diodes in a common anode arrangement, in accordance with some embodiments. The pulsed laser diode drivers 401-404 each generally include the source resistor R_(S), the source capacitor C_(S), the damping resistor R_(Damp), the inductor L_(s), the bypass capacitor C_(BP), two or more laser diodes D_(L) ¹ - D_(L) ^(n), and the bypass switch M_(BP). The pulsed laser diode drivers 401-402 each include two or more laser diode switches M_(DL) ¹ - M_(DL) ^(n), whereas the pulsed laser diode drivers 403-404 include a single laser diode switch M_(DL) ¹

Also shown is the controller 120, nodes 410, 412, respective parasitic inductances L_(DL) ¹ - L_(DL) ^(n) of the laser diodes D_(L) ¹ - D_(L) ^(n), the DC input voltage V_(in), the source voltage V_(S) at the source capacitor C_(S), the current i_(LS) through the inductor L_(S), respective currents i_(DL) ¹ - i_(DL) ^(n) through the laser diodes D_(L) ¹ - D_(L) ^(n), and the bypass switch gate driver signal GATE_(BP). The pulsed laser diode drivers 401-402 each utilize respective laser diode switch gate driver signals GATE_(DL) ¹ - GATE_(DL) ^(n), whereas the pulsed laser diode drivers 403-404 use a single laser diode switch gate driver signal GATE_(DL) ¹. Electrical connections of the pulsed laser diode drivers 401-404 are similar to, or the same as, those described with respect to the pulsed laser diode drivers 101-103. Topologies of the pulsed laser diode drivers 401-404 vary with respect to the placement of the bypass capacitor C_(BP).

As shown in the simplified circuit schematics of the pulsed laser diode driver 401 of FIG. 4A and the pulsed laser diode driver 404 of FIG. 4D, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to the anodes of the laser diodes D_(L) ¹ - D_(L) ^(n). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in the simplified circuit schematic of the pulsed laser diode drivers 402-403 of FIGS. 4B-C, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor Ls and to the respective anodes of the laser diodes D_(L) ¹- D_(L) ^(n). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp). In some embodiments, values of the DC input voltage V_(in), inductance of the inductor L_(S), capacitance of the source capacitor C_(S), resistance of the damping resistor R_(Damp), and capacitance of the bypass capacitor C_(BP) are similar to, or the same as, those respective values as described with reference to the pulsed laser diode drivers 101-103. However, the values of the DC input voltage V_(in), inductance of the inductor L_(S), capacitance of the source capacitor C_(S), resistance of the damping resistor R_(Damp), and capacitance of the bypass capacitor C_(BP) can advantageously be selected to achieve desired operation of the pulsed laser diode drivers 401-404 (e.g., a charge time, a pulse width, a pulse voltage, a pulse current level). Operation of the pulsed laser diode drivers 401-404 is similar to, or the same as, operation of the pulsed laser diode drivers 101-103 as explained in detail with respect to the simplified plots 201-206 of FIGS. 2A-D, as well as the example switching sequence 300 shown in FIG. 3 .

In some embodiments, the controller 120 is configured to determine how many of the laser diodes D_(L) ¹ - D_(L) ^(n) are enabled simultaneously and to adjust a voltage level of the DC input voltage V_(in) in accordance with that determination to supply a required amount of current (e.g., using a digitally adjustable voltage source (described below) controlled by a digital control signal from the controller 120).

FIGS. 5A-D are simplified circuit schematics of pulsed laser diode drivers 501-504 of a third general topology that is configured to drive a laser diode using a high-side switch, in accordance with some embodiments. The pulsed laser diode drivers 501-504 each generally include the source resistor R_(S), the source capacitor C_(S), the damping resistor R_(Damp), the inductor L_(S), the bypass capacitor C_(BP), the laser diode D_(L), the bypass switch M_(BP), and the laser diode switch M_(DL). The laser diode switch M_(DL) is configured as a high-side switch.

Also shown is the controller 120, nodes 510, 512, the parasitic inductance L_(DL) of the laser diode D_(L), the DC input voltage V_(in), the source voltage V_(S) at the source capacitor C_(S), the current i_(LS) through the inductor L_(S), the current i_(DL) through the laser diode D_(L), the bypass switch gate driver signal GATE_(BP), and the laser diode switch gate driver signal GATE_(DL). Most of the electrical connections of the pulsed laser diode drivers 501-504 are similar to, or the same as, those described with respect to the pulsed laser diode drivers 101-103. However, in contrast to the low-side configuration of the pulsed laser diode drivers 101-103, the drain node of the laser diode switch M_(DL) is directly electrically connected to the second terminal of the inductor L_(S) and to the drain node of the bypass switch M_(BP). The source node of the laser diode switch M_(DL) is directly electrically connected to the anode of the laser diode D_(L), and the cathode of the laser diode D_(L) is directly electrically connected to the bias voltage node. Topologies of the pulsed laser diode drivers 501-504 vary with respect to placement of the bypass capacitor C_(BP).

As shown in the simplified circuit schematic of the pulsed laser diode driver 501 of FIG. 5A, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to the drain node of the laser diode switch M_(DL). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in the simplified circuit schematic of the pulsed laser diode driver 502 of FIG. 5B, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the source node of the laser diode switch M_(DL) and to the anode of the laser diode D_(L). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in the simplified circuit schematic of the pulsed laser diode driver 503 of FIG. 5C, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S), to the drain node of the bypass switch M_(BP), and to the drain node of the laser diode switch M_(DL). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp). As shown in the simplified circuit schematic of the pulsed laser diode driver 504 of FIG. 5D, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the source node of the laser diode switch M_(DL) and the anode of the laser diode D_(L). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp).

FIGS. 6A-D are simplified circuit schematics of pulsed laser diode drivers 601-604 of a fourth general topology that is configured to drive two or more laser diodes in a common cathode configuration using a high-side switch, in accordance with some embodiments. The pulsed laser diode drivers 601-604 each generally include the source resistor R_(S), the source capacitor C_(S), the damping resistor R_(Damp), the inductor L_(S), the bypass capacitor C_(BP), the bypass switch M_(BP), two or more laser diodes D_(L) ¹ - D_(L) ^(n), and two or more respective laser diode switches M_(DL) ¹ - M_(DL) ^(n).

Also shown is the controller 120, nodes 610, 612, 614, respective parasitic inductances L_(DL) ¹ - L_(DL) ^(n) of the laser diodes D_(L) ¹ - D_(L) ^(n), the DC input voltage Vi_(n), the source voltage Vs at the source capacitor Cs, the current i_(LS) through the inductor Ls, respective currents i_(DL) ¹ - i_(DL) ^(n) through the laser diodes D_(L) ¹ - D_(L) ^(n), the bypass switch gate driver signal GATE_(BP), and respective laser diode switch gate driver signals GATE_(DL) ¹ -GATE_(DL) ^(n) of the laser diode switches M_(DL) ¹ - M_(DL) ^(n).

Most of the electrical connections of the pulsed laser diode drivers 601-604 are similar to, or are the same as, those described with respect to the pulsed laser diode drivers 501-504. However, topologies of the pulsed laser diode drivers 601-604 vary from one another with respect to placement of the bypass capacitor C_(BP).

As shown in the simplified circuit schematic of the pulsed laser diode driver 601 of FIG. 6A, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to respective drain nodes of the laser diode switches M_(DL) ¹ - M_(DL) ^(n) and the bypass switch M_(BP). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in the simplified circuit schematic of the pulsed laser diode driver 602 of FIG. 6B, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the source node of any of the laser diode switches (M_(DL) ^(n) is shown) and to the anode of the laser diode coupled to that laser diode switch (D_(L) ^(n) is shown). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. In some embodiments, multiple bypass capacitors C_(BP) are be used, each of the bypass capacitors being connected across a respective laser diode. As shown in the simplified circuit schematic of the pulsed laser diode driver 603 of FIG. 6C, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to respective drain nodes of the laser diode switches M_(DL) ¹ - M_(DL) ^(n) and the bypass switch M_(BP). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp). As shown in the simplified circuit schematic of the pulsed laser diode driver 604 of FIG. 6D, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the source node of any of the laser diode switches (M_(DL) ¹ is shown) and to the anode of the laser diode coupled to that laser diode switch (D_(L) ¹ is shown). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp). In some embodiments, multiple bypass capacitors C_(BP) are be used, each of the bypass capacitors C_(BP) having a first terminal that is directly electrically connected to a respective anode of each laser diode and a second terminal that is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(S).

In some embodiments, the controller 120 is operable to determine how many of the laser diodes D_(L) ¹ - D_(L) ^(n) are enabled simultaneously and to adjust a voltage level of the DC input voltage V_(in) in accordance with that determination to supply a required amount of current (e.g., using a digitally adjustable voltage source (described below) controlled by a digital control signal from the controller 120).

FIGS. 7A-E are simplified circuit schematics of pulsed laser diode drivers 701-705 of a fifth general topology that is configured to drive a laser diode using a half-bridge configuration, in accordance with some embodiments. The pulsed laser diode drivers 701-704 each generally include the source resistor R_(S), the source capacitor C_(S), the damping resistor R_(Damp), the inductor L_(S), the bypass capacitor C_(BP), the bypass switch M_(BP), the laser diode D_(L), and the laser diode switch M_(DL). The pulsed laser diode driver 705 additionally includes two or more laser diodes D_(L) ¹ - D_(L) ^(n), rather than the single laser diode D_(L), each of the two or more laser diodes D_(L) ¹ - D_(L) ^(n) having a respective parasitic inductance L_(DL) ¹ - L_(DL) ^(n), and respective current representation i_(DL) ¹ - i_(DL) ^(n). However, the pulsed laser diode driver 705 lacks independent control of the two or more laser diodes D_(L) ¹ - D_(L) ^(n).

Also shown is the controller 120, nodes 710, 712, the parasitic inductance L_(DL) of the laser diode D_(L), the DC input voltage V_(in), the source voltage V_(S) at the source capacitor C_(S), the current i_(LS) through the inductor L_(S), the current i_(DL) through the laser diode D_(L), the currents i_(DL) ¹-i_(DL) ^(n) through the two or more laser diodes D_(L) ¹ - D_(L) ^(n), the bypass switch gate driver signal GATE_(BP), and the laser diode switch gate driver signal GATE_(DL) of the laser diode switch M_(DL).

Most of the electrical connections of the pulsed laser diode drivers 701-704 are similar to, or the same as those described with respect to the pulsed laser diode drivers 501-503. However, in contrast to the high-side configuration of the pulsed laser diode drivers 501-503, the drain node of the bypass switch M_(BP) is directly electrically connected to the source node of the laser diode switch M_(DL) and to the anode of the laser diode D_(L). The source node of the bypass switch M_(BP) is directly electrically connected to the bias voltage node. Thus, as shown in the simplified circuit schematics of the pulsed laser diode drivers 701-704, the laser diode D_(L) may be driven by the half-bridge configuration of the bypass switch M_(BP) and the laser diode switch M_(DL). Topologies of the pulsed laser diode drivers 701-704 vary with respect to placement of the bypass capacitor C_(BP).

As shown in the simplified circuit schematic of the pulsed laser diode driver 701 of FIG. 7A, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to the drain node of the laser diode switch M_(DL). In such embodiments, the second terminal of the bypass capacitor C_(BP) is electrically connected to the bias voltage node. As shown in the simplified circuit schematic of the pulsed laser diode driver 702 of FIG. 7B, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the source node of the laser diode switch M_(DL), to the drain node of the bypass switch M_(BP), and to the anode of the laser diode D_(L). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in the simplified circuit schematic of the pulsed laser diode driver 703 of FIG. 7C, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and to the drain node of the laser diode switch M_(DL). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp). As shown in the simplified circuit schematic of the pulsed laser diode driver 704 of FIG. 7D, in some embodiments the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the source node of the laser diode switch M_(DL), the drain node of the bypass switch M_(BP), and the anode of the laser diode D_(L). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor Cs and to the first terminal of the damping resistor R_(Damp).

As shown in the simplified circuit schematic of the pulsed laser diode driver 705 of FIG. 7E, two or more laser diodes D_(L) ¹ - D_(L) ^(n) may be driven simultaneously by the half-bridge configuration of the bypass switch M_(BP) and the laser diode switch M_(DL). In the example shown, the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S) and the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp). However, other configurations of the bypass capacitor C_(BP), such as those described with reference to FIGS. 7A-D may be used.

FIGS. 8A-B are simplified circuit schematics of pulsed laser diode drivers 801-802 of a sixth general topology that is configured to drive a laser diode using a high-side switch, in accordance with some embodiments. The pulsed laser diode drivers 801-802 generally include the source resistor R_(S), the source capacitor C_(S), the damping resistor R_(Damp), the inductor L_(S), the bypass capacitor C_(BP), the laser diode D_(L), the bypass switch M_(BP), and the laser diode switch M_(DL). Also shown is the controller 120, nodes 810, 812, the respective parasitic inductances L_(DL) of the laser diode D_(L), the DC input voltage V_(in), the source voltage V_(S) at the source capacitor C_(S), the current i_(LS) through the inductor L_(S), the current i_(DL) through the laser diodes D_(L), the bypass switch gate driver signal GATE_(BP), and the laser diode switch gate driver signal GATE_(DL). Electrical connections of the pulsed laser diode driver 801 are similar to, or the same as those described with respect to the pulsed laser diode driver 101. The pulsed laser diode drivers 801-802 differ in that the drain node of the laser diode switch M_(DL) is directly electrically connected to the second terminal of the source resistor R_(S) and to the first terminal of the source capacitor C_(S). The source node of the laser diode switch M_(DL) is directly electrically connected to the first terminal of the inductor L_(S). The anode of the laser diode D_(L) is directly electrically connected to the second terminal of the inductor L_(S) and the cathode of the laser diode D_(L) is directly electrically connected to the bias voltage node. As shown, the pulsed laser diode drivers 801-802 are advantageously configured such that the laser diode switch M_(DL) is electrically connected between the inductor L_(S) and the source capacitor C_(S). As a result, the drain node of the laser diode switch M_(DL) does not receive a high voltage spike developed at the second terminal of the inductor L_(S) when the bypass switch M_(BP) is disabled to generate the high-current pulse through the laser diode D_(L).

The pulsed laser diode drivers 801-802 differ in placement of the bypass capacitor C_(BP). As shown in FIG. 8A, in some embodiments, the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S), to the anode of the laser diode D_(L), and to the drain node of the bypass switch M_(BP). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in FIG. 8B, in some embodiments, the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S), to the anode of the laser diode D_(L), and to the drain node of the bypass switch M_(BP). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp).

In other embodiments, the respective positions of the inductor L_(S) and the laser diode switch M_(DL) in either of the pulsed laser diode drivers 801-802, can be exchanged such that the first terminal of the inductor L_(S) is directly electrically connected to the first terminal of the source capacitor Cs, and the drain terminal of the laser diode switch M_(DL) is directly electrically connected to the second terminal of the inductor L_(S).

FIGS. 9A-B are simplified circuit schematics of pulsed laser diode drivers 901-902 of a seventh general topology that is configured to drive a laser diode using only a bypass switch, in accordance with some embodiments. The pulsed laser diode drivers 901-902 generally include the source resistor Rs, the source capacitor C_(S), the damping resistor R_(Damp), the inductor L_(S), the bypass capacitor C_(BP), the laser diode D_(L), and the bypass switch M_(BP). Also shown are nodes 910, 912, the respective parasitic inductances L_(DL) of the laser diode D_(L), the DC input voltage V_(in), the source voltage V_(S) at the source capacitor C_(S), the current i_(LS) through the inductor Ls, the current i_(DL) through the laser diodes D_(L), and the bypass switch gate driver signal GATE_(BP). Electrical connections of the pulsed laser diode drivers 901-902 are similar to, or the same as, those described with respect to the pulsed laser diode driver 101. The pulsed laser diode drivers 901-902 differ in that the laser diode switch M_(DL) is eliminated. The anode of the laser diode D_(L) is directly electrically connected to the second terminal of the inductor Ls and the cathode of the laser diode D_(L) is directly electrically connected to the bias voltage node. In such embodiments, the voltage level of the DC input voltage V_(in) is restricted to a voltage level that does not surpass the forward bias voltage of the laser diode D_(L), thereby maintaining the laser diode D_(L) in an OFF-state (i.e., not conducting) until a voltage higher than the forward bias voltage is developed at the second terminal of the inductor L_(S) when current flow through the bypass switch is momentarily disabled.

The pulsed laser diode drivers 901-902 differ in placement of the bypass capacitor C_(BP). As shown in FIG. 9A, in some embodiments, the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S), to the anode of the laser diode D_(L), and to the drain node of the bypass switch M_(BP). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the bias voltage node. As shown in FIG. 9B, in some embodiments, the first terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the inductor L_(S), to the anode of the laser diode D_(L), and to the drain node of the bypass switch M_(BP). In such embodiments, the second terminal of the bypass capacitor C_(BP) is directly electrically connected to the second terminal of the source capacitor C_(S) and to the first terminal of the damping resistor R_(Damp).

Embodiments of the pulsed laser diode drivers disclosed herein are additionally or alternatively operable to provide current pulses to devices other than laser diodes. For instance, embodiments of the pulsed laser diode drivers disclosed herein are operable to provide a current pulse to a light-emitting diode (i.e., a non-laser LED). Additionally, embodiments of the pulsed laser diode drivers disclosed herein are operable to provide a current pulse to another circuit or device, having no laser diode, that is configured to receive a current pulse for a purpose other than emitting light.

In some embodiments, two or more instances of the laser diode drivers disclosed herein are configured to drive respective laser diodes. For example, four instances of the pulsed laser diode driver 802 may be used to drive a laser diode package that includes four laser diodes. In such an embodiment, each of the laser diodes in the laser diode package is driven by an instance of the pulsed laser diode driver 802.

FIGS. 10A-10B are simplified circuit schematics of pulsed laser diode drivers 1002/1004 of an eighth general topology that is configured for multi-channel, individual control of multiple laser diodes, in accordance with some embodiments. The multi-channel pulsed laser diode driver 1002 shown in FIG. 10A is configured to independently drive n laser diodes where n is a number ranging from two to 128 or more. The multi-channel pulsed laser diode driver 1002 is operable to cause a pulse to be emitted from any individual laser diode of the multi-channel pulsed laser diode driver 1002 in isolation, or combined with one or more other pulses emitted from other laser diodes of the multi-channel pulsed laser diode driver 1002. The multi-channel pulsed laser diode driver 1002 generally includes n source resistors R_(S) ¹ through R_(S) ^(n), n source capacitors C_(S) ¹ through C_(S) ^(n), an optional damping resistor R_(Damp), n inductors L_(S) ¹ through L_(S) ^(n), n bypass switches M_(BP) ¹ through M_(BP) ^(n), n bypass capacitors C_(BP) ¹ through C_(BP) ^(n), n laser diodes D_(L) ¹ through D_(L) ^(n), and a laser diode switch M_(DL), coupled as shown. Also shown is the controller 120 discussed above, respective parasitic inductances L_(DL) ¹ through L_(DL) ^(n) of the laser diodes D_(L) ¹ through D_(L) ^(n), respective currents i_(LS) ¹ through i_(LS) ^(n) of the inductors L_(S) ¹ through L_(S) ^(n), respective currents i_(DL) ¹ through i_(DL) ^(n) of the laser diodes D_(L) ¹ through D_(L) ^(n), and the DC input voltage V_(in). The damping resistor R_(Damp) is used in some embodiments for current measurement purposes and can be omitted by connecting each of the source capacitors C_(S) ¹ through C_(S) ^(n) to ground. In some embodiments, the bypass switches M_(BP) ¹ through M_(BP) ^(n) and the laser diode switch M_(DL) are each N-type FET switches and advantageously do not require bootstrap circuitry to drive the respective gates of those switches because of their respective low-side configurations.

The source resistor R_(S) ¹, the source capacitor C_(S) ¹, the inductor L_(S) ¹, the bypass switch M_(BP) ¹ _(,) the bypass capacitor C_(BP) ¹, and the laser diode D_(L) ¹ are associated with a first channel of the multi-channel pulsed laser diode driver 1002. Similarly, the source resistor R_(S) ^(n), the source capacitor C_(S) ^(n), the inductor L_(S) ^(n), the bypass switch M_(BP) ^(n), the bypass capacitor C_(BP) ^(n), and the laser diode D_(L) ^(n) are associated with an n^(th) channel of the multi-channel pulsed laser diode driver 1002, where n is a number greater than one (e.g., two, three, four, eight, 16, 32, 64, 128, etc.). By controlling (e.g., by the controller 120) respective switch timings (i.e., an on/off duration) of the bypass switches M_(BP) ¹ through M_(BP) ^(n) in conjunction with controlling a switch timing of the laser diode switch M_(DL) each of the laser diodes D_(L) ¹ through D_(L) ^(n) are advantageously independently controlled. Operation of each channel of the multi-channel pulsed laser diode driver 1002 is similar to, or the same as, operation of the pulsed laser diode driver 101 described with reference to FIG. 1A and the switching sequence 300 shown in FIG. 3 . Because each of the bypass switches M_(BP) ¹ through M_(BP) ^(n) and the laser diode switch M_(DL) are configured as low-side switches (i.e., a source node of each aforementioned switch is directly electrically connected to ground), a gate control signal of those switches does not need to be level-shifted by bootstrap circuitry, thereby advantageously simplifying the design and reducing the cost of the multi-channel pulsed laser diode driver 1002 as compared to a laser diode driver circuit that requires bootstrap circuitry.

An example embodiment of a four-channel (i.e., n = 4) multi-channel pulsed laser diode driver 1004 is shown in FIG. 10B. The multi-channel pulsed laser diode driver 1004 is operable to independently drive four laser diodes. That is, the multi-channel pulsed laser diode driver 1004 is operable to cause a pulse to be emitted from any individual laser diode of the multi-channel pulsed laser diode driver 1004 in isolation, or combined with one or more other pulses emitted from other laser diodes of the multi-channel pulsed laser diode driver 1004. The multi-channel pulsed laser diode driver 1004 generally includes four source resistors Rs¹ through Rs⁴, four source capacitors C_(S) ¹ through C_(S) ⁴, the optional damping resistor R_(Damp), four inductors Ls¹ through Ls⁴, four bypass switches M_(BP) ¹ through M_(BP) ⁴, four bypass capacitors C_(BP) ¹ through C_(BP) ⁴, four laser diodes D_(L)1 through D_(L) ⁴, and the laser diode switch M_(DL), directly electrically connected as shown. Also shown is the controller 120, respective parasitic inductances L_(DL) ¹ through L_(DL) ⁴ of the laser diodes D_(L) ¹ through D_(L) ⁴, the DC input voltage V_(in), nodes 1011 through 1014, and nodes 1021 through 1024. The damping resistor R_(Damp) is used in some embodiments for current measurement purposes and can be omitted by connecting each of the source capacitors C_(S) ¹ through C_(S) ⁴ to ground. In some embodiments, the bypass capacitors C_(BP) ¹ through C_(BP) ⁴ are connected to the cathodes of the laser diodes D_(L) ¹ through D_(L) ⁴. In some embodiments, the bypass switches M_(BP) ¹ through M_(BP) ⁴ and the laser diode switch M_(DL) are each N-type FET switches and advantageously do not require boot-strap circuitry to drive the respective gates of those switches as described above.

The source resistor Rs ¹, the source capacitor Cs¹, the inductor Ls¹, the bypass switch M_(BP) ¹, the bypass capacitor C_(BP) ¹, and the laser diode D_(L) ¹ are associated with a first channel of the multi-channel pulsed laser diode driver 1004; the source resistor Rs², the source capacitor C_(S) ², the inductor Ls², the bypass switch M_(BP) ², the bypass capacitor C_(BP) ², and the laser diode D_(L) ² are associated with a second channel of the multi-channel pulsed laser diode driver 1004; the source resistor Rs³, the source capacitor C_(S) ³, the inductor Ls³, the bypass switch M_(BP) ³, the bypass capacitor C_(BP) ³, and the laser diode D_(L) ³ are associated with a third channel of the multi-channel pulsed laser diode driver 1004, and the source resistor Rs⁴, the source capacitor C_(S) ⁴, the inductor Ls⁴, the bypass switch M_(BP) ⁴, the bypass capacitor C_(BP) ⁴, and the laser diode D_(L) ⁴ are associated with a fourth channel of the multi-channel pulsed laser diode driver 1004. The laser diode switch M_(DL) is associated with each of the channels of the multi-channel pulsed laser diode driver 1004.

As described above, each channel of the multi-channel pulsed laser diode driver 1004 has an associated source resistor, source capacitor, inductor, bypass switch, bypass capacitor, and laser diode. By controlling (e.g., by the controller 120) respective switch timings (i.e., an on/off duration) of the bypass switches M_(BP) ¹ through M_(BP) ⁴ in conjunction with controlling a switch timing of the laser diode switch M_(DL), each of the laser diodes D_(L) ¹ through D_(L) ⁴ is advantageously independently controlled.

Operation of each channel of the multi-channel pulsed laser diode driver 1004 is similar to, or the same as operation of the pulsed laser diode driver 101 described with reference to FIG. 1A and the switching sequence 300 shown in FIG. 3 . A channel of the multi-channel pulsed laser diode driver 1004 is selected for output by turning that channel’s bypass switch off (e.g., by the controller 120) while the laser diode switch M_(DL) is off such that the DC input voltage V_(in) charges that channel’s source capacitor to a desired voltage level to store energy in that source capacitor (e.g., step 301 of FIG. 3 ). After the desired voltage level is reached at the source capacitor, a selected channel’s bypass switch is turned on (e.g., by the controller 120), such that current builds in that channel’s inductor between that channel’s bypass switch and that channel’s source capacitor (e.g., step 302 of FIG. 3 ). If that channel’s bypass switch is thereafter turned off for a short time and the laser diode switch M_(DL) is turned on, that channel’s inductor current will resonate with the anode capacitance of that channel’s laser diode, thereby creating a voltage across that channel’s laser diode that is higher than the DC input voltage V_(in) and the developed current will be forced to flow through that channel’s laser diode (e.g., step 303 of FIG. 3 ) to emit a laser pulse. In some embodiments, a discharge sequence similar to step 304 of FIG. 3 is performed, whereby both that channel’s bypass switch and the laser diode switch M_(DL) are turned on may then follow. By sequentially selecting each channel of the multi-channel laser diode driver 1004, that channel’s laser diode can be independently pulsed. A channel of the multi-channel pulsed laser diode driver 1004 is unselected for output by leaving that channel’s bypass switch on (e.g., by the controller 120) through each of the steps 301 through 305 shown in FIG. 3 , thereby preventing the DC input voltage V_(in) from charging that channel’s source capacitor.

Simplified example waveforms 1102 of signals related to the operation of the multi-channel pulsed laser diode driver 1004 are shown in FIG. 11 , in accordance with some embodiments. Also shown is a legend 1101 and expanded regions of interest 1104, 1106, 1108, and 1110 of the waveforms 1102.

As indicated by the legend 1101, the simplified waveforms 1102 of FIG. 11 include a laser diode switch gate driver signal Gate_(DL), a first bypass switch gate driver signal Gate_(BP) ¹, a second bypass switch gate driver signal Gate_(BP) ², a third bypass switch gate driver signal Gate_(BP) ³ and a fourth bypass switch gate driver signal Gate_(BP) ⁴ over a 20 µs duration. With reference to FIG. 10B, the laser diode switch gate driver signal Gate_(DL) is operable to control the laser diode switch M_(DL), the first bypass switch gate driver signal Gate_(BP) ¹ is operable to control the bypass switch M_(BP) ¹, the second bypass switch gate driver signal Gate_(BP) ² is operable to control the bypass switch M_(BP) ², the third bypass switch gate driver signal Gate_(BP) ³ is operable to control the bypass switch M_(BP) ³, and the fourth bypass switch gate driver signal Gate_(BP) ⁴ is operable to control the bypass switch M_(BP) ⁴.

Each of the expanded regions of interest 1104, 1106, 1108, and 1110 illustrate a pre-flux interval of a selected channel during which an inductor current of that channel’s inductor is ramping up, a very short pulse interval during which current through that channel’s inductor is directed through that channel’s laser diode, and a discharge interval in accordance with steps 301 through 305 described with reference to FIG. 3 . Per the description above, the region of interest 1104 illustrates pulse generation for the first channel (i.e., laser diode D_(L) ¹) of the multi-channel laser diode driver 1004, the region of interest 1106 illustrates pulse generation for the second channel (i.e., laser diode D_(L) ²) of the multi-channel laser diode driver 1004, the region of interest 1108 illustrates pulse generation for the third channel (i.e., laser diode D_(L) ³) of the multi-channel laser diode driver 1004, and the region of interest 1110 illustrates pulse generation for the fourth channel (i.e., laser diode D_(L) ²) of the multi-channel laser diode driver 1004.

Additional simplified example waveforms 1202 of signals related to the operation of the multi-channel pulsed laser diode driver 1004 of FIG. 10B are shown in FIG. 12 . The simplified example waveforms include waveforms 1211 through 1214 illustrating respective anode voltages of the laser diodes D_(L) ¹ through D_(L) ⁴ at the nodes 1011 through 1014, and waveforms 1221 through 1224 illustrating respective voltages of the source capacitor C_(S) ¹ through C_(S) ⁴ at the nodes 1021 through 1024. Also shown are waveforms 1231 through 1234 which illustrate when a respective channel of the multi-channel pulsed laser diode driver 1004 is enabled.

As shown, when a first channel of the multi-channel pulsed laser diode driver 1004 is enabled (illustrated by waveform 1231), an anode voltage 1211 at node 1011 of the laser diode D_(L) ¹ rises in conjunction with a rising voltage at node 1021 of the source capacitor C_(S) ¹. Upon enabling the laser diode switch M_(DL) and momentarily disabling the bypass switch M_(BP) ¹, current flows through the laser diode D_(L) ¹, thereby emitting a laser pulse as described above. Similarly, when a second channel of the multi-channel pulsed laser diode driver 1004 is enabled (illustrated by waveform 1232), an anode voltage 1212 at node 1012 of the laser diode D_(L) ² rises in conjunction with a rising voltage at node 1022 of the source capacitor C_(S) ². Upon enabling the laser diode switch M_(DL) and momentarily disabling the bypass switch M_(BP) ², current flows through the laser diode D_(L) ², thereby emitting a laser pulse as described above. Operation of the third and fourth channels of the multi-channel laser diode driver 1004 are similar.

A repetition rate of the multi-channel pulsed laser diode driver 1004, as well as each of the pulsed laser diode drivers described above, is limited by a charging time of each channel’s source capacitor. The pulsed laser diode drivers described above create narrow (e.g., 1-5nsec) high-current pulses (e.g., 40amp) through a driven laser diode. The instantaneous power in the driven laser diode is therefore high (e.g., in the order of hundreds of watts). However, for many applications (e.g., Lidar), the duty cycle of the pulse is generally 0.01% or less to limit the total power dissipated in the laser diode which results in an upper limit to a repetition rate. In conventional laser diode driver applications, a resistor is used to charge storage (i.e., source) capacitors during each cycle. In such conventional solutions, an RC time constant of such charging circuits is typically not an issue because the duty cycle is so low. However, for applications that require a high repetition rate for laser pulses, the RC time constant of conventional charging circuits creates an undesirable limitation. In any of the embodiments disclosed herein, each source resistor of a given pulsed laser diode driver may be advantageously replaced by an actively controlled source switch that quickly charges an associated source capacitor. Activation of the source switch is synchronized with switching the one or more bypass switches and one or more laser diode switches of a given pulsed laser diode driver such that the source switch is enabled prior to a laser diode pulse generation interval. FIG. 13A through FIG. 13I provide examples of previously described laser diode drivers in which the respective source resistor R_(S) has been replaced by an actively controlled source switch M_(S) to rapidly charge the respective source capacitor C_(S). In some embodiments, the actively controlled source switch is implemented as a P-type switch which advantageously does not require bootstrap circuitry. Respective actively controlled source switches M_(S) shown in FIG. 13A through FIG. 13I are activated only during a pre-charge step (i.e., during step 301 as described with reference to FIG. 3 ), and thus prior to a pre-flux step (i.e., prior to step 302 as described with reference to FIG. 3 ).

FIG. 13A shows a first example embodiment of a pulsed laser diode driver 1301 having all of the components, signals, and nodes described above with reference to the pulsed laser diode driver 101 of FIG. 1A, with the exception of the source resistor R_(S) of FIG. 1A which has advantageously been replaced in FIG. 13A by an actively controlled (e.g., by the controller 120 using gate control signal GATEs) source switch Ms to rapidly charge the source capacitor C_(S). In other example embodiments (not shown), the respective source resistors Rs of the pulsed laser diode driver 102 of FIG. 1B and the pulsed laser diode driver 103 of FIG. 1C are similarly replaced by a respective actively controlled source switch to rapidly charge the respective source capacitors C_(S) of the laser diode drivers 102/103.

FIG. 13B shows a second example embodiment of a pulsed laser diode driver 1302 having all of the components, signals, and nodes described above with reference to the pulsed laser diode driver 401 of FIG. 4A, with the exception of the source resistor Rs of FIG. 4A which has advantageously been replaced in FIG. 13B by an actively controlled (e.g., by the controller 120 using gate control signal GATEs) source switch M_(S) to rapidly charge the source capacitor C_(S). In other example embodiments (not shown), the respective source resistors Rs of the pulsed laser diode driver 402 of FIG. 4B, the pulsed laser diode driver 403 of FIG. 4C, and the pulsed laser diode driver 404 of FIG. 4D are similarly replaced by a respective actively controlled source switch to rapidly charge the respective source capacitors C_(S) of the laser diode drivers 402/403/404.

FIG. 13C shows a third example embodiment of a pulsed laser diode driver 1303 having all of the components, signals, and nodes described above with reference to the pulsed laser diode driver 501 of FIG. 5A, with the exception of the source resistor Rs of FIG. 5A which has advantageously been replaced in FIG. 13C by an actively controlled (e.g., by the controller 120 using gate control signal GATEs) source switch M_(S) to rapidly charge the source capacitor Cs. In other example embodiments (not shown), the respective source resistors Rs of the pulsed laser diode driver 502 of FIG. 5B, the pulsed laser diode driver 503 of FIG. 5C, and the pulsed laser diode driver 504 of FIG. 5D are similarly replaced by a respective actively controlled source switch to rapidly charge the respective source capacitors C_(S) of the laser diode drivers 502/503/504.

FIG. 13D shows a fourth example embodiment of a pulsed laser diode driver 1304 having all of the components, signals, and nodes described above with reference to the pulsed laser diode driver 601 of FIG. 6A, with the exception of the source resistor Rs of FIG. 6A which has advantageously been replaced in FIG. 13D by an actively controlled (e.g., by the controller 120 using gate control signal GATEs) source switch M_(S) to rapidly charge the source capacitor C_(S). In other example embodiments (not shown), the respective source resistors Rs of the pulsed laser diode driver 602 of FIG. 6B, the pulsed laser diode driver 603 of FIG. 6C, and the pulsed laser diode driver 604 of FIG. 6D are similarly replaced by a respective actively controlled source switch to rapidly charge the respective source capacitors C_(S) of the laser diode drivers 602/603/604.

FIG. 13E shows a fifth example embodiment of a pulsed laser diode driver 1305 having all of the components, signals, and nodes described above with reference to the pulsed laser diode driver 701 of FIG. 7A, with the exception of the source resistor Rs of FIG. 7A which has advantageously been replaced in FIG. 13E by an actively controlled (e.g., by the controller 120 using gate control signal GATEs) source switch M_(S) to rapidly charge the source capacitor C_(S). In other example embodiments (not shown), the respective source resistors Rs of the pulsed laser diode driver 702 of FIG. 7B, the pulsed laser diode driver 703 of FIG. 7C, the pulsed laser diode driver 704 of FIG. 7D, and the pulsed laser diode driver 705 of FIG. 7E are similarly replaced by a respective actively controlled source switch to rapidly charge the respective source capacitors C_(S) of the laser diode drivers 702/703/704/705.

FIG. 13F shows a sixth example embodiment of a pulsed laser diode driver 1306 having all of the components, signals, and nodes described above with reference to the pulsed laser diode driver 801 of FIG. 8A, with the exception of the source resistor Rs of FIG. 8A which has advantageously been replaced in FIG. 13F by an actively controlled (e.g., by the controller 120 using gate control signal GATEs) source switch M_(S) to rapidly charge the source capacitor C_(S). In other example embodiments (not shown), the source resistor Rs of the pulsed laser diode driver 802 of FIG. 8B is similarly replaced by an actively controlled source switch to rapidly charge the source capacitor C_(S) of the pulsed laser diode driver 802.

FIG. 13G shows a seventh example embodiment of a pulsed laser diode driver 1307 having all of the components, signals, and nodes described above with reference to the pulsed laser diode driver 901 of FIG. 9A, with the exception of the source resistor Rs of FIG. 9A which has advantageously been replaced in FIG. 13G by an actively controlled (e.g., by the controller 120 using gate control signal GATEs) source switch M_(S) to rapidly charge the source capacitor Cs. In other example embodiments (not shown), the source resistor Rs of the laser diode driver 902 of FIG. 9B is similarly replaced by an actively controlled source switch to rapidly charge the source capacitor Cs of the laser diode driver 902.

FIG. 13H shows an eighth example embodiment of a pulsed laser diode driver 1308 having all of the components, signals, and nodes described above with reference to the multi-channel pulsed laser diode driver 1002 of FIG. 10A, with the exception of the source resistors R_(S) ¹ though R_(S) ^(n) of FIG. 10A which have advantageously been replaced in FIG. 13H by respective actively controlled (e.g., by the controller 120 using gate control signals GATE_(S) ¹ through GATE_(S) ^(n)) source switches M_(S) ¹ through M_(S) ^(n) to rapidly charge the source capacitors C_(S) ¹ through C_(S) ^(n).

FIG. 13I shows a ninth example embodiment of a pulsed laser diode driver 1309 having all of the components, signals, and nodes described above with reference to the multi-channel pulsed laser diode driver 1004 of FIG. 10B, with the exception of the source resistors R_(S) ¹ through R_(S) ⁴ of FIG. 10B which have advantageously been replaced in FIG. 13I by respective actively controlled (e.g., by the controller 120 using gate control signals GATE_(S) ¹ through GATE_(S) ⁴) source switches M_(S) ¹ through M_(S) ⁴ to rapidly charge the source capacitors C_(S) ¹ through C_(S) ⁴.

Simplified example waveforms 1402 of signals related to the operation of the multi-channel pulsed laser diode driver 1309 of FIG. 13I are shown in FIG. 14 , in accordance with some embodiments. The simplified example waveforms 1402 include waveforms 1421 through 1424 illustrating respective voltages across the source capacitor C_(S) ¹ through C_(S) ⁴ at nodes 1021 through 1024 of FIG. 13I, respectively. Also shown are waveforms 1431 through 1434 which illustrate when a respective channel of the multi-channel pulsed laser diode driver 1309 is enabled, a clock signal 1441, and high-current pulses 1451 through 1455. As shown, the multi-channel pulsed laser diode driver 1309 is operable to emit a high-current pulse 1451 through 1455 to drive a respective laser diode D_(L) ¹ through D_(L) ⁴, a pulse being emitted every 10 µs. The examples shown in FIGS. 13A-13I are merely select examples of pulsed laser diode driver circuits configured to advantageously use a source switch (i.e., M_(S)) for rapid charging of a source capacitor (i.e., C_(S)). In some embodiments, any of the pulsed laser diode drivers 101-103, 401-404, 501-504, 601-604, 701-705, 801-802, 901-902, 1002-1004 are configured to use a source switch (i.e., M_(S)) instead of a source resistor (i.e., Rs) to rapidly charge a source capacitor (i.e., C_(S)).

FIG. 15 shows a simplified circuit schematic of a pulsed laser diode driver 1501 of a ninth general topology, in accordance with some embodiments. The pulsed laser diode driver 1501 generally includes a source switch M_(S), a source capacitor C_(S), a damping resistor R_(Damp), an inductor L_(S), a bypass capacitor C_(BP), a laser diode D_(L), a bypass switch M_(BP), and a flux switch M_(FLUX). The flux switch M_(FLUX) is configured as a low-side switch. Also shown is the controller 120, node 110, a parasitic inductance L_(DL) of the laser diode D_(L), a DC input voltage V_(in), a source voltage V_(s) at the source capacitor C_(S), a current i_(LS) through the inductor L_(S), a current i_(DL) through the laser diode D_(L), a bypass switch gate driver signal GATE_(BP), and a flux switch gate driver signal GATE_(FLUX).

As shown in FIG. 15 , a first terminal of the source switch M_(S) is directly electrically connected to the DC input voltage V_(in). In other embodiments (not shown), the source switch M_(S) may be replaced with a source resistor Rs. A second terminal of the source switch M_(S) is directly electrically connected to a first terminal of the source capacitor C_(S). A second terminal of the source capacitor C_(S) is directly electrically connected to a bias voltage node such as ground. The second terminal of the source switch M_(S) is directly electrically connected to a cathode of the laser diode D_(L), a first terminal of the damping resistor R_(Damp), a first terminal of the bypass capacitor C_(BP), and a first terminal of the inductor L_(S). A second terminal of the damping resistor R_(Damp) is directly electrically connected to a first terminal of the flux switch M_(FLUX), and a second terminal of the flux switch M_(FLUX) is directly electrically connected to a bias voltage node such as ground. An anode of the laser diode D_(L) is directly electrically connected to a second terminal of the bypass capacitor C_(BP), a second terminal of the inductor L_(S), and to a first terminal of the bypass switch M_(BP). A second terminal of the bypass switch M_(BP) is directly electrically connected to a bias voltage node such as ground.

The bypass switch M_(BP) is configured to receive the bypass switch gate driver signal GATE_(BP) at a gate node (e.g., from the controller 120), the bypass switch gate driver signal GATE_(BP) being operable to turn the bypass switch M_(BP) on or off based on a voltage level of the bypass switch gate driver signal GATE_(BP). The source switch Ms is configured to receive the source switch gate driver signal GATE_(S) at a gate node (e.g., from the controller 120), the source switch gate driver signal GATE_(S) being operable to turn the source switch M_(S) on or off based on a voltage level of the source switch gate driver signal GATEs. Similarly, the flux switch M_(FLUX) is configured to receive the flux switch gate driver signal GATE_(FLUX) at a gate node (e.g., from the controller 120), the flux switch gate driver signal GATE_(FLUX) being operable to turn the flux switch M_(FLUX) on or off based on a voltage level of the flux switch gate driver signal GATE_(FLUX). Any or all of the bypass switch M_(BP), the source switch M_(S), and/or the flux switch M_(FLUX) can be implemented as N-type switches or P-type switches. In some embodiments, the bypass switch M_(BP), the source switch Ms, and/or the flux switch M_(FLUX) are implemented as Silicon-based or Silicon-Carbide-based field-effect transistors (FETs).

In some embodiments, the pulsed laser diode driver 1501 is configured to receive the DC input voltage V_(in) having a voltage range from about 10 V to 20 V, which is advantageously lower than an input voltage used by many conventional pulsed laser diode drivers. The inductor Ls is a physical component added to the pulsed laser diode driver 1501 (i.e., as opposed to a representation of a parasitic inductance caused by components or interconnections such as bond wires). Similarly, the bypass capacitor C_(BP) is a physical component added to the pulsed laser diode driver 1501 (i.e., as opposed to a representation of a parasitic capacitance). One advantage of using physical inductor and capacitor components rather than using parasitic inductances and capacitances is that values of the inductor L_(S) and the bypass capacitor C_(BP) can be easily modified by a designer or even an end-user. By comparison, conventional designs that rely on parasitic reactances may require re-design and/or re-layout to change an operating parameter.

As disclosed herein, values of the DC input voltage V_(in), the inductance of the inductor Ls, the capacitance of the source capacitor C_(S), the resistance of the damping resistor R_(Damp), and the capacitance of the bypass capacitor C_(BP) can advantageously be selected (“tuned”) to achieve a desired operation of the pulsed laser diode driver 1501 (e.g., a charge time, a pulse width, a pulse voltage, a pulse current). For example, a pulse width of the current i_(DL) flowing through the laser diode D_(L) can be tuned by adjusting the capacitance value of the bypass capacitor C_(BP). A peak current level of the pulse of current i_(DL) flowing through the laser diode D_(L) can be tuned by adjusting the source voltage V_(s) on the supply capacitor C_(S). A capacitance value of the source capacitor C_(S) can be tuned to adjust a timing delay of the high-current pulse and an upper range of the current i_(DL) through the laser diode D_(L). Resistance values of the damping resistor R_(Damp) are dependent on the capacitance value of the supply capacitor C_(S) and can be tuned within a range of values such that at a lower resistance, a lower frequency resonance of the pulsed laser diode drivers disclosed herein is underdamped (e.g., at about R_(Damp) = 0.1 Ohm), or is critically damped (e.g., at about R_(Damp) = 0.4 Ohm). The damping resistor R_(Damp) is operable to prevent current of the generated resonant waveform from becoming negative which could thereby enable a body diode of the bypass switch M_(BP) or the flux switch M_(FLUX). Although a resulting maximum current level of the current i_(DL) through the laser diode D_(L) is lower for the critically damped case, the current level can be easily adjusted by raising the voltage level of the DC input voltage V_(in).

In some embodiments, the DC input voltage V_(in) is about 15 V, the inductance of the inductor L_(S) is about 6 nH, the capacitance of the source capacitor C_(S) is about 100 nF, the resistance of the damping resistor R_(Damp) is about 0.1 Ohm, and the capacitance of the bypass capacitor C_(BP) is about 1 nF. In some embodiments, a voltage at the first terminal of the damping resistor R_(Damp) is received by the controller 120 to provide an indication of a current flow through the damping resistor R_(Damp).

Typical resonant driver designs often require a damping resistor to minimize ringing duration. However, the added damping resistor R_(Damp) dissipates power which may lower the overall power efficiency of the design as compared to a resonant driver that does not have a damping resistor. Thus, in some embodiments, the pulsed laser diode driver 1501 advantageously allows current to flow through the damping resistor R_(Damp) during portions of a switching sequence (e.g., the switching sequence 300) in which the damping resistor R_(Damp) critically damps ringing, and prevents current from flowing through the damping resistor R_(Damp) during portions of the switching sequence when the damping resistor R_(Damp) is not needed to damp ringing. The pulsed laser diode driver 1501 allows current to flow through the damping resistor R_(Damp) by enabling the flux switch M_(FLUX) and prevents current from flowing through the damping resistor R_(Damp) by disabling the flux switch M_(FLUX). Such dynamic control of current flow through the damping resistor R_(Damp) advantageously increases an overall power efficiency of the pulsed laser diode driver 1501 as compared to a pulsed laser diode driver circuit that allows current to flow through a damping resistor for the entirety of a switching sequence.

During operation, the source capacitor C_(S) is discharged through the inductor L_(S) by the bypass switch M_(BP). This configuration provides a maximum peak current through the laser diode D_(L), but requires the series damping resistor R_(Damp) to prevent the waveform from ringing for a long duration. Until the ringing stops and the voltage and current are zero, the bypass switch M_(BP) cannot be turned off. Unfortunately, the damping resistor R_(Damp) dissipates power as long as current flows through the damping resistor R_(Damp). Thus, the pulsed laser diode driver 1501 advantageously provides an optimal power efficiency by preventing current from flowing through the damping resistor R_(Damp) during an initial precharge step (e.g., step 301 of FIG. 3 ), a preflux step (e.g., step 302 of FIG. 3 ), and a pulse generation step (e.g., step 303 of FIG. 3 ) of a switching sequence (e.g., the switching sequence 300 of FIG. 3 ). However, current is allowed, by the flux switch M_(FLUX), to flow through the damping resistor R_(Damp) after the high-current pulse has been generated (e.g., at step 303 of FIG. 3 ) to remove remaining ringing by critically damping the RLC network of the pulsed laser diode driver 1501.

During the precharge step (e.g., step 301 of FIG. 3 ), the preflux step (e.g., step 302 of FIG. 3 ), and the pulse generation step (e.g., step 303 of FIG. 3 ) of the switching sequence (e.g., the switching sequence 300 of FIG. 3 ), the flux switch M_(FLUX) is disabled, thereby creating an undamped LC network. However, after pulse generation, the flux switch M_(FLUX) is enabled and the damping resistor R_(Damp) creates a parallel RLC network to critically damp ringing and thereby provide a maximum power efficiency and fast recovery of the pulsed laser diode driver 1501 to start a next switching sequence.

For example, FIGS. 16A-16B show simplified plots, 1620 a-b, 1621 a-b, 1622 a-b, 1623 a-b, 1624 a-b, and 1625 a-b, of signals related to operation of the pulsed laser diode driver 1501 shown in FIG. 15 , in accordance with some embodiments. In particular, FIG. 16A illustrates operation of the pulsed laser diode driver 1501 when a damping resistor (i.e., the damping resistor R_(Damp)) underdamps ringing of the pulsed laser diode driver 1501. In comparison, FIG. 16B illustrates operation of the pulsed laser diode driver 1501 when a damping resistor (i.e., the damping resistor R_(Damp)) is used to critically damp ringing of the pulsed laser diode driver 1501.

With reference to FIGS. 16A-16B, the simplified plots illustrate voltage plots of the bypass switch gate driver signal GATE_(BP) 1620 a-b, voltage plots of the flux switch gate driver signal GATE_(FLUX) 1621 a-b, current plots of the current i_(LS) through the inductor L_(S) 1622 a-b, current plots of the current i_(DL) through the laser diode D_(L) 1623 a-b, voltage plots of the source voltage Vs 1624 a-b at the source capacitor C_(S), and voltage and current plots 1625 a-b of a voltage and current source used to establish a plot scale, all over the same duration of time. Details of these signals are described below. The voltage plots of the bypass switch gate driver signal GATE_(BP) 1620 a-b and the flux switch gate driver signal GATE_(FLUX) 1621 a-b have been level-shifted for readability, but are, in actuality, low voltage inputs. Additionally, the voltage plots of the bypass switch gate driver signal GATE_(BP) 1620 a-b and the flux switch gate driver signal GATE_(FLUX) 1621 a-b assume that the flux switch M_(FLUX) and the bypass switch M_(BP) are NFET devices. However, if PFET devices are used instead, the polarity of the bypass switch gate driver signal GATE_(BP) 1620 a-b and the flux switch gate driver signal GATE_(FLUX) 1621 a-b are inverted.

In the example shown in FIG. 16A, with reference to FIG. 15 , a resistance value of 10 Ohms is used for the damping resistor R_(Damp) of the pulsed laser diode driver 1501 in which Ls = 6 nH, and C_(BP) = 1nF, and L_(DL) is about 1 nH. As expected, the waveforms 1622 a and 1624 a are very underdamped as shown by prolonged oscillations (i.e., “ringing”). As is known in the art, for a parallel RLC circuit, the damping coefficient d is expressed as:

$\begin{matrix} {d = \frac{1}{2R} \times \sqrt{\frac{L}{C}}} & \text{­­­(Equation 1)} \end{matrix}$

Thus, if a critically damped waveform is desired, an optimal resistance R value of the damping resistor R_(Damp) can be determined by setting the damping coefficient d in Equation 1 to a value of d = 1 and solving Equation 1 for R using the values mentioned above. In the example shown in FIG. 16B, a resistance value of 0.175 Ohms is used for the damping resistor R_(Damp) of the pulsed laser diode driver 1501. As expected, the waveforms 1622 b and 1624 b are thereby critically damped as shown by the absence of prolonged oscillations (i.e., “ringing”).

In some embodiments, the damping resistor R_(Damp) can be eliminated by using a weak switch having an on-resistance Rdson that is about the desired resistance value determined using Equation 1. In such embodiments, if adjustment of the resistance value is desired, a segmented FET can be used to thereby allow the on-resistance Rdson to be modified to match the damping resistance required.

Additionally, although it would initially appear that placing the source capacitor C_(S) in series with the laser diode D_(L) would raise the required anode voltage to pulse the laser diode D_(L), the voltage and current of the source capacitor C_(S) are 90 \-degrees out of phase with one another. As shown by waveforms 1624 a-b, because the current pulse (i.e., 1623 a-b) through the laser diode D_(L) is advantageously aligned with a peak current amplitude, voltage at the source capacitor C_(S) at that time is zero due to the 90 \-degree phase shift. In some embodiments, a beginning of the high-current pulse could be determined by sensing when the source voltage V_(S) at the source capacitor C_(S) is at zero, at which point the high-current pulse through the laser diode D_(L) should begin.

For some applications, the amplitude of a high-current pulse delivered by a resonant circuit such as any of those disclosed herein may need to be adjusted in amplitude from pulse-to-pulse. Thus, in some embodiments, any of the pulsed laser drivers disclosed herein are advantageously operable to configure an amplitude of the high-current pulse delivered to one or more laser diodes on a pulse-to-pulse basis.

As shown in FIG. 17 , FIG. 18 , FIG. 19 , and FIG. 20 , the DC input voltage V_(in) is advantageously provided by an adjustable voltage supply (i.e., a digital-to-analog converter (DAC)). In some embodiments, an output voltage level of the adjustable voltage supply is set using the controller 120. For example, FIG. 17 illustrates a pulsed laser diode driver circuit 1701 that is the same as the pulsed laser diode driver 101 shown in FIG. 1A with the exception that the DC input voltage V_(in) is generated by a DAC 1730. FIG. 18 illustrates a pulsed laser diode driver circuit 1801 that is the same as the pulsed laser diode driver 1301 shown in FIG. 13A with the exception that the DC input voltage V_(in) is generated by a DAC 1830. FIG. 19 illustrates a pulsed laser diode driver circuit 1901 that is the same as the pulsed laser diode driver 1308 shown in FIG. 13H with the exception that the DC input voltage V_(in) is generated by a DAC 1930. FIG. 20 illustrates a pulsed laser diode driver circuit 2001 that is the same as the pulsed laser diode driver 1501 shown in FIG. 15 with the exception that the DC input voltage V_(in) is generated by a DAC 2030. The examples shown in FIG. 17 , FIG. 18 , FIG. 19 , and FIG. 20 are merely select examples of pulsed laser diode driver circuits configured to receive a DC input voltage from an adjustable voltage source (e.g., a DAC or a different adjustable voltage source as is known in the art). In some embodiments, any of the pulsed laser diode drivers 101-103, 401-404, 501-504, 601-604, 701-705, 801-802, 901-902, 1002-1004, 1301-1309, and/or 1501 are configured to receive the DC input voltage V_(in) from an adjustable voltage source such as a DAC.

Use of an adjustable voltage supply, such as a DAC, to provide the DC input voltage V_(in) to the pulsed laser diode driver circuits disclosed herein is possible because of the advantageously low input voltage requirements for such embodiments. In some embodiments, the adjustable voltage supply is clocked such that the adjustable voltage supply charges the source capacitor C_(S) described herein only during a first portion of a clock period (e.g., a positive portion). As such, the value of the DC input voltage V_(in) and a current amplitude of the high-current pulse delivered to the laser diode(s) disclosed herein may be advantageously varied between consecutive high-current pulses through the laser diode(s).

FIGS. 21A-21B show simplified plots, 2102 a-b, 2104 a-b, 2106 a-b, of signals related to operation of the pulsed laser diode drivers shown in FIGS. 17, 18, 19, and 20 , in accordance with some embodiments.

FIG. 21A includes examples of high-current pulses 2102 a (i.e., through the laser diode(s) D_(L)), a source voltage V_(S) at the source capacitor C_(S) 2106 a, and a linearly varying supply voltage 2106 a of a variable input voltage supply (e.g., a DAC) that provides the DC input voltage V_(in). As shown, a current amplitude of the high-current pulses 2102 a is advantageously varied from pulse to pulse.

FIG. 21B includes examples of high-current pulses 2102 b (i.e., through the laser diode(s) D_(L)), a source voltage V_(S) at the source capacitor C_(S) 2106 b, and a stepped supply voltage of a variable input voltage supply (e.g., a DAC) that provides the DC input voltage V_(in). As shown, a current amplitude of the high-current pulses 2102 b is advantageously varied from pulse to pulse. Although an output voltage transition of the variable input voltage supply is fast, change in the source voltage level V_(S) at the source capacitor C_(S) 2106 b is limited by the time constant of the source capacitor C_(S) and an on-resistance of an input switch (e.g., the source switch M_(S) described above) or an input resistor (e.g., the source resistor R_(S) described above).

Reference has been made in detail to embodiments of the disclosed invention, one or more examples of which have been illustrated in the accompanying figures. Each example has been provided by way of explanation of the present technology, not as a limitation of the present technology. In fact, while the specification has been described in detail with respect to specific embodiments of the invention, it will be appreciated that those skilled in the art, upon attaining an understanding of the foregoing, may readily conceive of alterations to, variations of, and equivalents to these embodiments. For instance, features illustrated or described as part of one embodiment may be used with another embodiment to yield a still further embodiment. Thus, it is intended that the present subject matter covers all such modifications and variations within the scope of the appended claims and their equivalents. These and other modifications and variations to the present invention may be practiced by those of ordinary skill in the art, without departing from the scope of the present invention, which is more particularly set forth in the appended claims. Furthermore, those of ordinary skill in the art will appreciate that the foregoing description is by way of example only, and is not intended to limit the invention. 

What is claimed is:
 1. A pulsed laser diode driver comprising: an inductor having a first terminal and a second terminal, the first terminal being configured to receive a source voltage; a source capacitor having a first capacitor terminal directly electrically connected to the first terminal of the inductor to provide the source voltage and a second capacitor terminal electrically coupled to a bias voltage node; a laser diode switch having a drain node that is directly electrically connected to the second terminal of the inductor; a first laser diode having an anode that is directly electrically connected to a source node of the laser diode switch and a cathode that is directly electrically connected to the bias voltage node; a bypass switch having a drain node that is directly electrically connected to the source node of the laser diode switch and a source node that is directly electrically connected to the bias voltage node; and a bypass capacitor having a first terminal that is directly electrically connected to the drain node of the laser diode switch; wherein: the laser diode switch and the bypass switch are configured to control a current flow through the inductor to produce a high-current pulse through the first laser diode, the high-current pulse corresponding to a peak current of a resonant waveform developed at the anode of the first laser diode.
 2. The pulsed laser diode driver of claim 1, wherein: a second terminal of the bypass capacitor is directly electrically connected to the bias voltage node.
 3. The pulsed laser diode driver of claim 1, wherein: a second terminal of the bypass capacitor is directly electrically connected to the second terminal of the source capacitor.
 4. The pulsed laser diode driver of claim 1, further comprising: a resistor configured to receive a DC input voltage, the source voltage being received at the first terminal of the source capacitor via the resistor.
 5. The pulsed laser diode driver of claim 1, wherein: the second terminal of the source capacitor is electrically coupled to the bias voltage node via a damping resistor.
 6. The pulsed laser diode driver of claim 1, wherein: the second terminal of the source capacitor is electrically coupled to the bias voltage node via a direct electrical connection to the bias voltage node.
 7. The pulsed laser diode driver of claim 1, wherein: the laser diode switch is a Silicon-based field-effect transistor.
 8. The pulsed laser diode driver of claim 1, further comprising: a source switch configured to receive a DC input voltage, the source voltage being received at the first terminal of the source capacitor via the source switch.
 9. The pulsed laser diode driver of claim 1, further comprising: a second laser diode having an anode that is directly electrically connected to the source node of the laser diode switch and a cathode that is directly electrically connected to the bias voltage node.
 10. A pulsed laser diode driver comprising: an inductor having a first terminal and a second terminal, the first terminal being configured to receive a source voltage; a source capacitor having a first capacitor terminal directly electrically connected to the first terminal of the inductor to provide the source voltage and a second capacitor terminal electrically coupled to a bias voltage node; a laser diode switch having a drain node that is directly electrically connected to the second terminal of the inductor; a first laser diode having an anode that is directly electrically connected to a source node of the laser diode switch and a cathode that is directly electrically connected to the bias voltage node; a bypass switch having a drain node that is directly electrically connected to the source node of the laser diode switch and a source node that is directly electrically connected to the bias voltage node; and a bypass capacitor having a first terminal that is directly electrically connected to the drain node of the bypass switch; wherein: the laser diode switch and the bypass switch are configured to control a current flow through the inductor to produce a high-current pulse through the first laser diode, the high-current pulse corresponding to a peak current of a resonant waveform developed at the anode of the first laser diode.
 11. The pulsed laser diode driver of claim 10, wherein: a second terminal of the bypass capacitor is directly electrically connected to the bias voltage node.
 12. The pulsed laser diode driver of claim 10, wherein: a second terminal of the bypass capacitor is directly electrically connected to the second terminal of the source capacitor.
 13. The pulsed laser diode driver of claim 10, further comprising: a resistor configured to receive a DC input voltage, the source voltage being received at the first terminal of the source capacitor via the resistor.
 14. The pulsed laser diode driver of claim 10, wherein: the second terminal of the source capacitor is electrically coupled to the bias voltage node via a damping resistor.
 15. The pulsed laser diode driver of claim 10, wherein: the second terminal of the source capacitor is electrically coupled to the bias voltage node via a direct electrical connection to the bias voltage node.
 16. The pulsed laser diode driver of claim 10, wherein: the laser diode switch is a Silicon-based field-effect transistor. 